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A Wheatstone bridge is a measuring instrument invented by Samuel Hunter Christie in 1833 and improved and popularized by Sir Charles Wheatstone in 1843. It is used to measure an unknown electrical resistance by balancing two legs of a bridge circuit, one leg of which includes the unknown component. Its operation is similar to the original potentiometer except that in potentiometer circuits the meter used is a sensitive galvanometer.## Derivation

## Significance

The Wheatstone bridge illustrates the concept of a difference measurement, which can be extremely accurate. Variations on the Wheatstone bridge can be used to measure capacitance, inductance, impedance and other quantities, such as the amount of combustible gases in a sample, with an explosimeter. The Kelvin double bridge was specially adapted from the Wheatstone bridge for measuring very low resistances. A "Kelvin one-quarter bridge" has also been developed. It has been theorized that a "three-quarter bridge" could exist; however, such a bridge would function identically to the Kelvin double bridge.## Modification of the fundamental bridge

The Wheatstone bridge is the fundamental bridge, but there are other modifications that can be made to measure various kinds of resistances when the fundamental Wheatstone bridge is not suitable. Some of the modifications are:## See also

## External links

In the circuit on the right, $R\_x$ is the unknown resistance to be measured; $R\_1$, $R\_2$ and $R\_3$ are resistors of known resistance and the resistance of $R\_2$ is adjustable. If the ratio of the two resistances in the known leg $(R\_2\; /\; R\_1)$ is equal to the ratio of the two in the unknown leg $(R\_x\; /\; R\_3)$, then the voltage between the two midpoints (B and D) will be zero and no current will flow through the galvanometer $V\_g$. $R\_2$ is varied until this condition is reached. The current direction indicates whether $R\_2$ is too high or too low.

Detecting zero current can be done to extremely high accuracy (see galvanometer). Therefore, if $R\_1$, $R\_2$ and $R\_3$ are known to high precision, then $R\_x$ can be measured to high precision. Very small changes in $R\_x$ disrupt the balance and are readily detected.

At the point of balance, the ratio of $R\_2\; /\; R\_1\; =\; R\_x\; /\; R\_3$

Therefore, $R\_x\; =\; (R\_2\; /\; R\_1)\; cdot\; R\_3$

Alternatively, if $R\_1$, $R\_2$, and $R\_3$ are known, but $R\_2$ is not adjustable, the voltage or current flow through the meter can be used to calculate the value of $R\_x$, using Kirchhoff's circuit laws (also known as Kirchhoff's rules). This setup is frequently used in strain gauge and Resistance Temperature Detector measurements, as it is usually faster to read a voltage level off a meter than to adjust a resistance to zero the voltage.

First, Kirchhoff's first rule is used to find the currents in junctions B and D: : :

- $I\_3\; -\; I\_x\; +\; I\_g\; =\; 0$

- $I\_1\; -\; I\_g\; -\; I\_2\; =\; 0$

Then, Kirchhoff's second rule is used for finding the voltage in the loops ABD and BCD:

- $(I\_3\; cdot\; R\_3)\; -\; (I\_g\; cdot\; R\_g)\; -\; (I\_1\; cdot\; R\_1)\; =\; 0$

- $(I\_x\; cdot\; R\_x)\; -\; (I\_2\; cdot\; R\_2)\; +\; (I\_g\; cdot\; R\_g)\; =\; 0$

The bridge is balanced and $I\_g\; =\; 0$, so the second set of equations can be rewritten as:

- $I\_3\; cdot\; R\_3\; =\; I\_1\; cdot\; R\_1$

- $I\_x\; cdot\; R\_x\; =\; I\_2\; cdot\; R\_2$

Then, the equations are divided and rearranged, giving:

- $R\_x\; =\; \{\{R\_2\; cdot\; I\_2\; cdot\; I\_3\; cdot\; R\_3\}over\{R\_1\; cdot\; I\_1\; cdot\; I\_x\}\}$

From the first rule, $I\_3\; =\; I\_x$ and $I\_1\; =\; I\_2$. The desired value of $R\_x$ is now known to be given as:

- $R\_x\; =\; \{\{R\_3\; cdot\; R\_2\}over\{R\_1\}\}$

If all four resistor values and the supply voltage ($V\_s$) are known, the voltage across the bridge ($V$) can be found by working out the voltage from each potential divider and subtracting one from the other. The equation for this is:

- $V\; =\; \{\{R\_x\}over\{R\_3\; +\; R\_x\}\}V\_s\; -\; \{\{R\_2\}over\{R\_1\; +\; R\_2\}\}V\_s$

This can be simplified to:

- $V\; =\; left(\{\{R\_x\}over\{R\_3\; +\; R\_x\}\}\; -\; \{\{R\_2\}over\{R\_1\; +\; R\_2\}\}right)V\_s$

The concept was extended to alternating current measurements by James Clerk Maxwell in 1865 and further improved by Alan Blumlein in about 1926.

- Strain gauge
- Potentiometer
- Potential divider
- Ohmmeter
- Resistance Temperature Detector
- Maxwell bridge

- Wheatstone Bridge - Interactive Java Tutorial National High Magnetic Field Laboratory
- efunda Wheatstone article
- Methods of Measuring Electrical Resistance - Edwin F. Northrup, 1912, full-text on Google Books

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Last updated on Wednesday October 08, 2008 at 07:15:33 PDT (GMT -0700)

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This article is licensed under the GNU Free Documentation License.

Last updated on Wednesday October 08, 2008 at 07:15:33 PDT (GMT -0700)

View this article at Wikipedia.org - Edit this article at Wikipedia.org - Donate to the Wikimedia Foundation

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